Creation of spin-triplet Cooper pairs in the absence of magnetic ordering
arXiv:1710.02161 · doi:10.1103/PhysRevLett.120.037701
Abstract
In superconducting spintronics, it is essential to generate spin-triplet Cooper pairs on demand. Up to now, proposals to do so concentrate on hybrid structures in which a superconductor (SC) is combined with a magnetically ordered material (or an external magnetic field). We, instead, identify a novel way to create and isolate spin-triplet Cooper pairs in the absence of any magnetic ordering. This achievement is only possible because we drive a system with strong spin-orbit interaction--the Dirac surface states of a strong topological insulator (TI)--out of equilibrium. In particular, we consider a bipolar TI-SC-TI junction, where the electrochemical potentials in the outer leads differ in their overall sign. As a result, we find that nonlocal singlet pairing across the junction is completely suppressed for any excitation energy. Hence, this junction acts as a perfect spin triplet filter across the SC generating equal-spin Cooper pairs via crossed Andreev reflection.
12 pages, 8 figures
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Cited by in corpus (20)
- Theory of Majorana zero modes in unconventional superconductors
- Anisotropic proximity-induced superconductivity and edge supercurrent in Kagome metal, K1-xV3Sb5
- Formation and detection of Majorana modes in quantum spin Hall trenches
- Crossed Andreev reflection in spin-polarized chiral edge states due to the Meissner effect
- Superconducting proximity effect in -wave cuprate/ graphene heterostructures
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- Spin-Valley Locking and Pure Spin-Triplet Superconductivity in Noncollinear Antiferromagnets Proximitized to Conventional Superconductors
- Odd-frequency Pairing in Josephson Junctions Coupled by Magnetic Textures